1997
DOI: 10.1117/12.279277
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Photoluminescence in poly(3-hexylthiophene)

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Cited by 8 publications
(20 citation statements)
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“…For pure P3HT the GSB decay constant is τ 1 = 440 ps and the fit of the P3HT/SWNT solution GSB decay gives τ 1 = 432 ps. These results are in accord with the P3HT singlet ( S 1 ) excited ‐state radiative decay of ∼500 ps as reported in the literature . For pristine P3HT, the decays of the features at 590 and 625 nm can also be fit with a single exponential decay giving τ 1 = 504 ps and τ 1 = 550 ps, respectively.…”
Section: Resultssupporting
confidence: 90%
“…For pure P3HT the GSB decay constant is τ 1 = 440 ps and the fit of the P3HT/SWNT solution GSB decay gives τ 1 = 432 ps. These results are in accord with the P3HT singlet ( S 1 ) excited ‐state radiative decay of ∼500 ps as reported in the literature . For pristine P3HT, the decays of the features at 590 and 625 nm can also be fit with a single exponential decay giving τ 1 = 504 ps and τ 1 = 550 ps, respectively.…”
Section: Resultssupporting
confidence: 90%
“…Also, mixtures of good and poor solvents have the capacity to generate a larger yield of aggregates than pure marginal solvents, which may impose limitations on the latter toward certain applications, such as optimizing the doping efficiency of P3HT . Despite these advantages of solvent mixtures, the available literature on the assembly and crystallization of P3HT in solvent mixtures is rather scarce, compared to those involving pure solvents . Furthermore, most of these endeavors exploit the fabrication of P3HT aggregates as a means to (1) manipulate the morphology of films and P3HT/nanoparticle composites, (2) affect charge transport and field effect mobility, or (3) study the structure and photophysics of the aggregates.…”
Section: Introductionmentioning
confidence: 99%
“…The two spectra (see Fig. ) have identical line‐shape, typical of P3HT in blends . This result demonstrates that the observed PL non‐uniformity are not related to any observable local composition variation, while the absence of F8BT PL demonstrates that efficient FRET energy transfer from F8BT to P3HT takes place in all the active film …”
Section: Discussionmentioning
confidence: 62%
“…The local PL spectra of a bright and a dark 20 μm × 20 μm region in the 579 nm map (see Fig. ) have different line‐shapes, with a higher intensity in the range 675 to 725 nm of the PL from dark regions at 579 nm (thus bright regions above 770 nm) . The line‐shape differences in the local PL spectra of rrP3HT evidences local non‐uniformity of the intermolecular interactions between rrP3HT molecules also affecting the F8BT‐P3HT mixing.…”
Section: Discussionmentioning
confidence: 96%
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